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Hamiltonian for this two-dimensional anharmonic oscillator has the form:
H = px2/2 + py2/2 +
wx2 x2/2 + wy2 y2/2 +
g(1/2) x y2,
where wx, wy are frequences of small harmonic normal-mode vibrations,
and g is a small perturbation parameter.
The energy is expanded in powers of g:
E(g) = E0 + E1 g + ...
+ EN gN, where
E0 = (nx + 1/2)wx
+ (ny + 1/2)wy is unperturbed harmonic-oscillator energy,
nx and ny
are the harmonic oscillator quantum numbers, and
N is the order of perturbation theory.
Download a text of the Mathematica program that is used for this calculation
19 coefficients for nx=9, ny=1, wx=1, wy=11/10 in exact form calculated earlier.
4 coefficients for nx=9, ny=1, wx=1 and arbitrary wy in exact form calculated earlier.
110 coefficients for wx=1, wy=1.1, and nx=0, nx=0, nx=0, nx=1, nx=0, nx=2, nx=0, nx=4, nx=1, nx=0, nx=1, nx=2, nx=2, nx=0, nx=2, nx=1, nx=2, nx=2, nx=3, nx=0, nx=3, nx=1, nx=4, nx=0, nx=5, nx=0, calculated earlier.
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